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Subject: Re: This Week's Damping Ring Discussions at the Sendai GDE Meeting
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From: Louis Emery <emery@aps.anl.gov>
To: "Mark A. Palmer" <map36@cornell.edu>
Cc: ilcdr@lbl.gov
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Date: Wed, 05 Mar 2008 01:58:21 -0600
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To all,

I agree with the relative scores in the tables.
I would weight the first table more. But I think
it would not change the order of the results.
I'm leaning towards the DCO cell structure because
of the reduced number of magnets, and I think the
DA problem is not insurmountable.

I missed the webex session on Tuesday, so I have some
comments and questions:

I'm not sure how the DCO lattice at 100 degrees/cell 
ended up with a (much?) smaller
dynamic aperture than the FODO5 lattice with 108 degree
per cell. I see that the cell length for DCO is shorter (making the
dispersion smaller) than the FODO5 FODO
cell, perhaps to partially compensate the larger I5 created by the
shorter and stronger dipole. I think the dynamic acceptance of FODO
cells with constant circumference should scale roughly as the cell
length squared. So a shorter dipole magnet resulted in a smaller dynamic
aperture.

Andy, was using a 2x field in the dipole for reducing the total dipole
magnet cost? Could the magnet be longer without disrupting
the mechanical layout much?

To rephrase a point by Aimin, if maintaining a 90 degree phase advance
is important for dynamic aperture, then an "upgrade" of momentum
compaction from 1.7e-4 to a value 25% lower can be done with the
conversion of the DCO cell to a TME-cell (keeping 90 degree
cell) by the insertion of one quad. This is, of course, at a cost of
192 magnets.

How does the lower symmetry of the DCO lattice affect the
dynamic aperture? Could we have the superconducting
stuff together in two groups at a 90 degree azimuth relative to 
the injection and extraction (like FODO4 but with doglegs added to
reduce heat load)? 

Thanks.
Louis Emery
